mm^m
rr-\'.
mm
Increased voltage phenomenon in a resonance circuit of unconventional
magnetic configuration
Osamu Ide
Clean Energy Laboratory, Natural Group Corporation, Shinagawa, Japan
(Received 11 November 1994; accepted for publication 24 February 1995)
The behavior of an LCR (inductance-capacitance-resistance) circuit with a movable ferromagnetic
core is discussed. The core is attracted by a magnetic field generated by an electric current resulting
from the discharge of a capacitor in the closed LCR circuit, An unusual increase in recharge voltage,
which was dependent on the magnetic configuration of the coil, was observed. This voltage increase
does not conform to the mathematical simulation of the system. The possibility that a positive
electromotive force was involved in this effect is discussed/ © 1995 American Institute of Physics.
I. INTRODUCTION
The author has btm developing a motor operated by the
discharge of a capacitor in an LCR (inductance-capacitance-
resistance) circuit. Unlike conventional do motors, this motor
utilizes die magnetic force of attraction between a current-
carrying coil and a movable ferromagnetic core. The force of
attraction between the two components resulting from the
capacitor discharge is converted to a rotary force. The uncon-
sumed magnetic energy is recycled as electrical energy by
recharging the capacitor,
In the course of developing this motor, it was discovered
that the recharge voltage depends on the precise configura-
tion of the system.
The purpose of this paper is to describe the increased
voltage phenomenon observed in the above system, A differ-
ential equation that expresses the phenomenon, as. well as
computer simulations, are also discussed.
It is appropriate here to briefly discuss other machines
based on a similar magnetic phenomenon. Many attempts
have hctn made to operate machinery that utilizes the non-
linear phenomenon of magnetism, such as ferroresonance 1,2
and parametric resonance. 3 The basic features of these ma-
chines is the magnetic saturation effect. The machines prima-
rily make use of the transition from a nonresonant state to a
resonant state, i.e., from the high inductance of a nonsat-
urated state to the low inductance of a saturated state, con-
verting these two modes to either oscillation or amplification.
It should be noted that the present system is completely
different from these machines, since there is no magnetic
saturation in the coils. Voltage changes found in the system
occur during the transition from a low-inductance state to a
high-inductance state, and are not subjected to the sudden
drop or rise typically associated with ferroresonance and
parametric resonance. In other words, other systems operate
in a closed magnetic field, whereas the system described here
operates in an open magnetic field. Electrically, this system
is basically closed, since the only power source used here is
a charged capacitor; it has no ac power supply such as that
used to operate other magnetic machines*
IK LCR CIRCUIT WITH AN INCREASE IN INDUCTANCE
The basis of the system discussed in the present paper is
a conventional LCR circuit. Figure 1(a) shows a basic LCR
circuit containing a capacitor initially charged to a voltage of
-f V . When the circuit is closed, the capacitor discharges its
energy through the inductor. The voltage and current in this
transient state are known to follow a damped oscillation [Fig,
Kb)].
Switch S can be replaced by a SCR (silicon controlled
rectifier) in order to eliminate switching loss [Fig. 2(a)]. The
other advantage of using the SCR is that a negative charge in
the capacitor is retained after discharge. The oscillation stops
after the first discharge, since the SCR automatically turns
off when the half-cycle current recharges capacitor C to a
recharge voltage of - V r . The voltage and current during this
process are shown in Fig. 2(b), The amount of recharge volt-
age is always smaller than the initial voltage due to tbi re-
sistance loss in the circuit.
The inductor (coil) in Fig. 2(a) is now replaced by two
separate coils that face each other, with a movable ferromag-
netic core inserted between the coils (Fig. 3). When the two
coils (electromagnets) L x and I^ are connected in series, they
generate magnetic fields that attract the ferromagnetic core
toward the coils.
Unlike when the core is fixed outside the coils (i.e., the
core has no influence on the coils), the approach of the core
results in an increase in combined inductance L, as well as
movement of the magnetic flux near the coils. This increase
in inductance and the movement of the flux naturally affect
the discharge current and recharge voltage.
Generally speaking, it is expected that the total recharge
voltage will decrease because this system produces mechani-
cal output as the core moves. However, through a series of
experiments, it was discovered that results depend on the
magnetic configuration of the coils used in the circuit. In
other words, for a certain land of magnetic field, the opposite
result could occur— an increase in the average current and
recharge voltage. To confirm the above observations, an ex-
periment was conducted, which is described in the following
section.
IN. INCREASED VOLTAGE PHENOMENON IN A LOR
CIRCUIT
A, Experimental method
The experimental setup is schematically shown in Fig. 4.
Ferromagnetic cores Mj and M 2 are attached to the rotor,
J. AppL Rhys, 77 (11), 1 June 1995
0021 -8979/95/77(1 1 )/60 1 6/6/$6.00
@ 1 995 American Institute of Physics 601 5
+Vo
(b)
which is driven by a dc motor. The cores can be rotated at
various speeds, with the speed of the axis being measured by
a tachometer. Four electromagnets, L t , 1^, L 3 » and L 4 are
connected in series and placed two-by~two in the stators fac-
ing each other. The number of turns, inductance (at 1 kHz),
and dc inductance of the coils are, respectively, 169, 7.76
mH, and 1.22 O. The magnetic field of the electromagnets
facing each other, L^L 3 and L 2 -L 4 , can either be attracting
(i.e., N-S, N~S) or opposing (i.e., N~S, S-N). The former state
will be called the "attracting mode" and the latter the "op-
posing mode." Placed between the two stators, each contain-
ing two electromagnets, is a rotor with two ferromagnetic
cores. The specific positions of the electromagnets and the
cores are schematically shown in Fig. 5.
At a certain distance between the coil and the core, com-
bined inductance is maximized. This position of the core will
be referred to as (he "reference point." The reference point
SCR
I
+Vo
Vc
R
jferromagnetic
core
FIG. 3. LCR circuit with two coils and a movable ferromagnetic core in-
serted between the coils.
will vary slightly, depending on the direction of the magnetic
fields. The reference point is exactly aligned with the elec-
tromagnets when the magnetic fields are attracting, and
slightly displaced when they are opposing.
Figure 6 shows how the inductance of the electromagnet,
measured by an LCR meter, is related to the displacement of
torquemeter
stator rotor stator
K I L
tachometer
*3ax!s
phase
sensor
SCR trigger unit
(a)
SCR trigger unit
current probe
capacitor
phase sensor
stator
rotor
FIG. 2. (a) LCR Circuit with a SCR instead of a switch, (b) Half-cycle
voltage and current oscillations of the circuit.
dc-motor torquemeter coil
(b)
FIG. 4. Experimental setup.
M«. 4-i HI Itr^A '(QOP;
Osarnu Ide
ferromagnetic rotor
core-
stator
opposing mode
attracting mode
(c)
FIG* 5. Specific geometry of the electromagnets and the ferromagnetic core:
(a) as viewed from the direction of the axis, (b) the cross section when cut
from Hne A to A', and (c) the stator and rotor at the reference points and the
discharge-initiation points.
the core from the electromagnet The force of attraction
(torque) between the electromagnet and the core is also in-
dicated, This L»d (inductance-displacement) curve shows
that the inductance gradually increases as the core ap-
proaches the magnet, reaching a maximum at the reference
point (d—0). It can seen from the figure that the rate of
change of inductance depends on the magnetic fields and is
greater in the attracting mode,
A discharge is initiated at the distance from the reference
point, at which the core can experience the maximum force
3(mH)
discharge starting point <-
Tq :1=3A
Tcjjgm) 33 (mH)
L
Tg <g-m)
10 20 30 40 50 60(mm)
d
(a)
30 40 50 60 (mm)
d
(b)
BIO. 6. Combined inductance (£) and torque (Tq) between the electromag-
net and the ferromagnetic core; The torque was measured under conditions
of constant current, Values of h and Tq for (a) the attracting mode, and (b)
the opposing mode.
J.AnnL Phva. UM 77 Klr> 11 1 .lima 1GQK
One rotation
of the rotor
FIG, 7. Voltage and current changes during one rotation of the rotor. The
SCR turn-on points are also indicated.
of attraction, Le,, L— 36.1 mH in the attracting mode and
L—29.9 mH in the opposing mode. The discharge is com-
pleted before the core reaches the reference point, indicating
that the rotor does not receive a negative torque from the
discharging coil
'The serial operation of the system (Fig. 7) is as follows:
(1) The capacitor is charged to -f V .
(2) When the ferromagnetic cores approach the electromag-
nets, SCR 3 is turned on and the capacitor is recharged to
(3) SCR 2 is then turned on and the capacitor is charged to
(4) The same cycle is repeated with the opposite 'current by
turning on SCR 4 and SCR 1 in succession (coils L 5 and
L 6 are used for protection from an overcharge current).
Thus, for each half rotation, the positive and negative dis-
charges are alternately repeated.
The positive and negative discharges are not completely
symmetrical. The conditions for each discharge are not ex-
actly the same due to the particular structure of the experi-
mental device, such as the shape, size, and position of the
core. This inevitably causes a slight difference in the
recharge-voltage efficiency between two opposite discharges,
This condition, however, applies to all cases examined.
Capacitance C is set at 15*87 jutF, and the initial voltage
Vq at ±240 V. The capacitor voltage was measured by a
high- voltage probe of 200 M(l (dc-^15 kHz) impedance, and
the current was measured by a clamp-type probe* Wave
forms of the capacitor voltage and the discharge current were
simultaneously recorded using a digital-storage oscilloscope
with a vertical resolution of 8 bits, (1/256; the scale ranges
from -320 to 4-320 V). Because of the dispersion of the
data, eight measurements of the positive and negative dis-
charges were recorded, and the averages were then exam-
ined. The estimated values was calculated by a computer
connected directly to the oscilloscope.
B* Estimation factors
One estimation factor is the return-voltage rate, desig-
nated as i\ This rate is defined according to the initial voltage
V and the recharge voltage ~~V r as
Dmitiii IrfA
ftm7
^iPi
C
Q
ts
fid
S
s |V>|/|Vb
(1)
Another factor is tlie apparent resistance jR, derived from
V , V r , and current L This value can foe deduced using the
following procedure. First, the energy relationship before (f
=0) and after (t—T/2) the discharge is known as
Eq — Ei^E r ,
(2)
where E is die initial electrostatic energy of the capacitor,
Ex the recharged electrostatic energy of the capacitor, and E r
the internal energy loss.
The values £ , E { , and E r are expressed, respectively,
as
Eo^CVl/2,
and
E
cm
r ^R Pdu
Jo
From these equations, R is written as
f-dt
/e=c(vg
-* /K
(3)
(4)
(5)
(6)
This value of JR indicates not only the resistance mea-
sured in the dc current but also includes the eddy current loss
and hysteresis loss, as well as the effect of back EMF (elec-
tromotive force). These resistances are generated when an
inductor interacts with a ferromagnetic core. In short, R can
be regarded as the total Joule loss of the inductor measured
in the ac system.
As mentioned in the previous section, the voltage-
current wave forms were accurately measured and recorded
by a digital storage oscilloscope. From these waves forms,
V , V r , and (Jftdt) can be calculated, and R can thus be
estimated,
C. Results
Figures 8 and 9 show the results of the experiments,
Return-voltage rate r and apparent resistance R are com-
pared at different rotor speeds from near zero to 400 r/min*
When the magnetic field is in the attracting mode, the
value of t follows a monotonic decreasing curve as the rotor
speed increases, Correspondingly, resistance R follows an
increasing curve, On the other hand, r is found to increase
slightly in the opposing mode, with a peak in the 50-100
r/min range, and then gradually decrease at faster speeds.
The values of JR follow an opposite curve.
IV. MATHEMATICAL ANALYSIS
In order to fully understand the above phenomenon, a
computer simulation of the relevant differential equation was
made.
To describe the model, inductance L should be replaced
by a time-dependent function L(t) that expresses the serial
change of L, It is clear that the combined inductance of the
0.62 _
o Vo > o
• Vo< o
a average
300 400
n (r/min)
FIG, 8, Results of the experiment—voltage return rate (r) for (a) the attract-
ing mode, and (b) the opposing mode.
electromagnet and the ferromagnetic core is related to the
speed at which the ferromagnetic core approaches the elec-
tromagnet*
In the experiment, discharge begins when the core expe-
riences the maximum torque, with the core traveling only a
very short distance. The change in inductance caused by this
motion may be regarded as linear over this narrow range.
Thus, the change in inductance can be expressed by the fol-
lowing equation;
L—L^ax (H),
(7)
where L is the initial inductance of the electromagnet (H)» a
the rate of inductance change over the distance (H/m), and x
the displacement of the core (m).
From x— v t, where v is the speed of the core and t is the
duration of discharge, Eq. (7) can be transformed, as follows:
L^L^avt (H).
(8)
The value aoQl s""" 1 ) in this equation is the rate of in-
ductance change over time. Since a is constant (unique to
each coil), this rate is proportional to v.
From Faraday's law, the voltage across coil Vj under
conditions of changing inductance L(r), is expressed as
^ttamn IHn
1
o Vo>
• Vo<
a average
. i
200
(b)
300 400
n (r/min)
FIG. 9. Results of the experiment—apparent resistance (R) for (a) the at-
tracting mode, and (b) the opposing mode.
Vi «d(Zr/)/df »d[(L + avt)I]fdt
**(L +avt)(dIldt) + avI; (9)
where v is a constant.
The terminal voltage of capacitor V c is expressed as
ff «(l/C) J Idt,
(10)
where C is a capacitance.
By applying Kirchhoff s law to V } , V c , and the voltage
resulting from resistance R and current I, the following equa-
tion is obtained:
(L +avt)(dUdt) + (UC)J Idt+(R + <xv)I°*0. (11)
This differential equation can be solved by using the
Runge-Kutta process with initial conditions f«0, V~V ,
and 7=0.
Figure 10 and Table I show the computer simulation of
the solution of this equation for the specific values of V , C>
a, v 9 and R 9 as compared with the experimental results. The
value of a is obtained from the slope of the L«d curve (Fig.
6) at L . The value of v is calculated from the core's rpm
(revolution per minute) and the traveling distance at one ro-
tation.
J* Appl. Phys., Vol. 77, No, 11, 1 Juno 1996
r (Vr/Vo)
0.62
7 -•- experiment
(n = 16) -
-^- calculation
0.81
r^ initial value
0,80
0.79
i . i . i . 1
100
r JVr/vkL
200
(a)
300 400
n (r/min)
0.82 _
0.81
0.80
0.79
experiment
(n = 16 )
calculation
100
200
(b)
300
400
n (r/min)
HG, 10, The computer simulation of the Eq. (11), as compared with the
experimental results: (a) the attracting mode, and .(b) the opposing mode.
The simulation predicts that the recharge voltage will
decrease as the core speed increases. This conforms well
with the experimental results in the attracting mode. In the
opposing mode, however, certain discrepancies can be found
between the simulation and the actual results.
V. DISCUSSION
The mathematical analysis in the previous section re-
veals that the recharge voltage decreases as the core speed
increases. With a constant core speed, it predicts that the
recharge voltage will decrease as a increases.
The reason for the decrease in the recharge voltage can
be given as follows. The displacement of the core during
discharge means there is a mechanical output in the system.
It is reasonable to conclude that the mechanical motion of
the core is compensated for by a decrease in recharge volt-
age. The cause of the increase in the apparent resistance R is
Oaamu Ide 6019
r
■■£■
:■»■■:
-O' ■■
Vo(V)
C(pF)
Lo(mH)
R (Q)
cc (H/m)
v (m/sec)
Fig.10(a)
attracting mode
240
15.87
36.1
6.41
0.285
0.01665 x n
Fig.10(b)
opposing mode
240
15.87
29.9
6.06
0.119
0.01 665 x n
considered to be the back EMF generated by the movement
of the core* For a constant rotor speed, it is clear that a coil
with a large a has a large attracting force.
However, the results differ in the case of the opposing
mode. Though a is positive, r increases over the range up to
a certain speed. After the peak, r decreases slightly but re-
mains greater than the initial value.
These results can be explained from the assumption that
the complex movement of. the Auk could generate a positive
EMF: the increase in the recharge voltage is due to an EMF
in the same direction as the discharge current, different from
the back EMF caused by Faraday's law*
The past controversy concerning electromagnetic induc-
tion might shed some light on this viewpoint. On this topic,
several authors have stated that the motional EMF caused by
the cutting of the magnetic lux and the induced EMF caused
by Faraday's law were independent phenomena. 4 * 5 These two
different types of EMF are generally expressed by the fol-
lowing equation:
V=-rf$/£ft+ (BXv)dL
/o
Jo
(12)
It can be postulated that these two types of EMF have
contradicting effects within the coil, and that the motional
EMF has a positive effect on the recharge voltage over a
certain range of core speed.
This hypothesis seems to be consistent with the results,
but is also highly speculative. It would be necessary to con-
firm its validity through further experimentation.
n (r/min)
VI. CONCLUSIONS
In this paper, the behavior of an LCR circuit with a mov-
able ferromagnetic core was discussed. The increase in the
inductance of the coil, which is caused by the attraction of
the core during discharge, yielded the following results.
(1) The recharge voltage is generally smaller when the core
moves than when it is stationary. The decrease m the
recharge voltage depends on the rate of change of the
inductance. The simulation based on the theoretical
equation confirmed the experimental results.
(2) When applying opposing magnetic fields to the facing
coils, an increase in the recharge voltage can be observed
in an electrically closed LCR circuit. The apparent resis-
tance of the coil decreased correspondingly.
(3) It can be postulated that the complex movement of mag-
netic flux generates a positive EMF, but the cause of the
voltage increase is not clear.
ACKNOWLEDGMENTS
This work was supported by the Natural Group Corpo-
ration. The author wishes to thank Dr. Takashi Aoki, Chubu
University, and Mr. Yoshihiko Tago, InterScience Co, Ltd.,
for their helpful suggestions and comments related to this
paper.
1 J. I Blakley, IEEE Trans. Magn. MAG-19, 1570 (1983),
2 B. H. Smith, 3EE 114, 1707 (1967).
3 S. KJkuchi, Y. Sakamoto, and K. Murakami, IEEE Trans. Magn. MAG-20,
1792 (1984).
4 G. Cohn, Electrical Eng. 68, 441 (1949),
5 P. Moon and D. Spencer, I Franklin Institute 260, 213 (1955).
6 J. C, West and B. V. Jayawant, Institution Electrical Eng. 109A, 292
(1962).
7 0. W. Swift, XEEE Trans. Power Apparatus Systems PAS«88, 42 (1989),
6020 J, Appl. Phys M Vol. 77, No. 11, 1 Juno 1995
Osamu Ida